Method for Manufacturing a Multimode Optical Fibre

Abstract

The invention relates to a multimode optical fibre having a refractive index profile, comprising a light-guiding core surrounded by one or more cladding layers. The present invention furthermore relates to an optical communication system comprising a transmitter, a receiver and a multimode optical fibre.

Description

FIELD OF THE INVENTION

The present invention relates to a multimode optical fibre having a refractive index profile, comprising a light-guiding core surrounded by one or more cladding layers. The present invention furthermore relates to an optical communication system comprising a transmitter, a receiver and a multimode optical fibre. In addition to that, the present invention relates to a method for manufacturing a multimode optical fibre having a refractive index profile, wherein doped or undoped glass layers are deposited on the interior of a substrate tube by means of a chemical vapour deposition technique, using a reactive gas mixture, so as to obtain a preform having a precisely defined refractive index profile, from which preform a multimode optical fibre is drawn by heating one end of the preform, as well as to a multimode optical fibre having a refractive index profile, comprising a light-guiding gradient index core built up from a number of dopant.

BACKGROUND OF THE INVENTION

A multimode optical fibre is known per se from U.S. Pat. No. 4,339,174, which employs a bandwidth of at least 700 MHz. The optical fibre that is known therefrom comprises three separate regions, viz. an outer cladding layer, a barrier layer disposed on the inside wall surface of the cladding layer, and a core of a very pure glass with a refractive index profile disposed within the barrier layer, wherein the core comprises SiO₂ doped with a sufficient amount of a first oxide for increasing the index of refraction of the core to a value higher than that of the cladding layer, wherein the first oxide concentration varies according to a specific profile. For a multimode optical fibre having a core diameter of 64.0 μm and a numerical aperture of 0.207, bandwidths (MHz) of 1024 and 1082 have been measured for wavelengths of 900 nm and 1300 nm, respectively. Further details with regard to the transmission capacity are not provided therein.

From U.S. Pat. No. 3,989,350 there is known a multimode optical fibre having a refractive index profile for modal dispersion reduction with a view to widening the usable bandwidth of an optical communication system. The multimode optical fibre that is known therefrom comprises a core having an index of refraction which radially decreases from the fibre axis to the region at the core circumference, the core essentially consisting of SiO₂ and at least one refractive index modifying substance, in particular a radially increasing concentration of boron oxide, wherein the final composition at the core circumference essentially comprises boron silicate containing from 10 mole percent B₂O₃ to 20 mole percent B₂O₃. Further details with regard to the bandwidth or the transmission capacity are not provided.

From U.S. Pat. No. 4,222,631 there is known a multimode optical fibre comprising at least three glass-forming compounds and having a core with a radially gradient refractive index profile and a cladding, wherein the refractive index profile varies according to a specific formula as a function of the radius. Specific details with regard to the bandwidth or the transmission capacity are not provided.

Because of the continuous growth in data communication and telecommunication, there is a need for communication systems and glass fibres having a high transmission capacity. One way of increasing the transmission capacity of a glass fibre (system) is to use so-called Wavelength Division Multiplexing (WDM), wherein several signals are simultaneously transmitted through a glass fibre at different wavelengths. Because of the expensive peripheral equipment that is needed, this technique is mainly used in long-distance networks, in which single mode fibres are used.

Also in local networks (LANs), storage networks (SANs) and connecting networks, however, in which multimode fibres are frequently used in view of the relatively short distances and the large number of connections, there is a growing need for a high transmission capacity to be realised by means of WDM techniques. In addition to that, there is a tendency to use lasers without temperature stabilisation in the aforesaid short-distance networks, which is significantly cheaper than using temperature-stabilised lasers. With such lasers without temperature stabilisation, a shift in the laser wavelength will take place in the case of temperature changes. Both the use of WDM techniques and the use of lasers that are not temperature-stabilized requires that the bandwidth of multimode fibres be sufficiently high over a relatively large wavelength range for the transmission rates that are to be used.

Multimode glass fibres having a high bandwidth suitable for high transmission rates can be produced by introducing a very precisely defined refractive index profile into the fibre. Previously published International application PCT/NL02/00604 filed in the name of the present applicant, for example, indicates that the refractive index profile of such fibres must be exactly in accordance with the equation according to formula (1):

$\begin{array}{cc}n\left(r\right)=n_1\sqrt{1-2{\Delta \left(\frac{r}{a}\right)}^{\alpha }}& \left(1\right)\end{array}$

wherein:

n₁=the refractive index value of the fibre core

r=the radial position in the fibre core (μm)

Δ=the refractive index contrast of the fibre

a=the profile shape parameter

a=the fibre core radius (μm)

Said International application furthermore indicates that an adequate control of the inner part of the optical core is important. Lasers are generally used with the desired high transmission rates, which lasers, because of the spot size, only “expose” part of the optical core, so that more stringent requirements are made as regards an adequate profile control.

According to the method that is known from PCT/NL02/00604 it is possible to produce multimode fibres having a high bandwidth at one particular wavelength for which the fibre was designed. Such a fibre is suitable for high transmission rates at that particular wavelength. When the fibre is used with wavelengths different from the design wavelength (both higher and lower), the bandwidth is significantly lower, as a result of which the maximum transmission rate is lower at wavelengths different from the design wavelength.

SUMMARY OF THE INVENTION

A first aspect of the present invention is to obtain multi-mode glass fibres that can be used over a relatively large wavelength range at a specific transmission rate.

According to another aspect of the present invention, the multimode fibres preferably have a specific core diameter and numerical aperture and a specific minimum Over Filled Launch (OFL) bandwidth, measured in accordance with FOTP-204, TIA/EIA-455-204.

Another aspect concerns the need for optical communication systems comprising a multimode fibre, which systems have a relatively large wavelength range at a specific transmission rate.

Yet another aspect of the present invention concerns the need for optical communication systems comprising multimode fibres, which systems make it possible to use lasers that are not temperature-stabilized.

Another aspect of the present invention is to provide an optical fibre having a sufficiently high bandwidth in a specific wavelength range, e.g. around 800 nm, for realising a specific transmission capacity.

Another aspect of the present invention comprises the provision of a multimode optical fibre that is compatible with the multi-mode fibres that are already installed.

According to the present invention, the multimode optical fibre as referred to in the introduction is characterized in that the transmission capacity is at least 1 Gbit/sec over a wavelength band having a width of at least 100 nm in a wavelength range comprising 1300 nm, and that over a fibre length of at least 1000 m.

According to another embodiment, the transmission capacity is at least 10 Gbit/sec over a wavelength band having a width of at least 50 nm, in particular a width of at least 100 nm, in a wavelength range comprising 850 nm, and that over a fibre length of at least 150 m.

A special embodiment of a multimode optical fibre according to the present invention is characterized in that the transmission capacity is at least 1 Gbit/sec over a wavelength band having a width of at least 250 nm in a wavelength range comprising 1400 nm, and that over a fibre length of at least 850 m.

Since it is very desirable that such multimode fibres are compatible with the multimode fibres that are already installed, the fibre preferably has a core diameter of 62.5 μm, the numerical aperture ranges from 0.25 to 0.30 and the minimum OFL bandwidth is at least 160 Mhz·km at 850 nm, more in particular, the minimum OFL bandwidth is at least 300 Mhz·km at 1300 nm.

The present invention further relates to a multimode optical fibre having a refractive index profile, comprising a light-guiding core surrounded by one or more cladding layers, which is characterized in that the transmission capacity is at least 1 Gbit/sec over a wavelength band having a width of at least 100 nm in a wavelength range comprising 1300 nm, and that over a fibre length of at least 2000 m.

In a special embodiment of a multimode optical fibre according to the present invention, the transmission capacity is at least 10 Gbit/sec over a wavelength band having a width of at least 50 nm, in particular a width of at least 100 nm, in a wavelength range comprising 850 nm, and that over a fibre length of at least 300 m.

According to yet another embodiment of the present invention, the transmission capacity of the multimode optical fibre is at least 1 Gbit/sec over a wavelength band having a width of at least 250 nm in a wavelength range comprising 1400 nm, and that over a fibre length of at least 1300 m.

Since it is very desirable that such fibres be compatible with the multimode fibres that are already installed, the fibre preferably has a core diameter of 50 μm, the numerical aperture ranges from 0.18 to 0.22 and the minimum OFL bandwidth is at least 400 Mhz·km at 850 nm, more in particular, the minimum OFL bandwidth is at least 400 Mhz·km at 1300 nm.

In order to be able to guarantee such transmission capacities of a graded index multimode optical fibre in various systems that may use lasers having different characteristics, certain models are available that define the minimum OFL bandwidth of the fibres to be used. The OFL bandwidths that are minimally required for the aforesaid combinations of transmission capacity/product/wavelength range are thus known to those skilled in the art.

Furthermore, the present optical fibres must not exhibit any perturbation in the central part of the DMD (Differential Mode Delay) characteristic in the wavelength range to be used. Such perturbations may include: double pulses, pulse widening, leading pulses or trailing pulses.

In the DMD measurement, the impulse response of the transmission of light pulses at different radial positions through the core of a multimode fibre is measured. When using an optical multimode fibre at the aforesaid higher transmission rates, it is important that the impulse response of the light pulses in the central portion of the fibre core having a diameter of 18 μm does not exhibit any perturbation.

The present invention furthermore relates to an optical communication system comprising a transmitter, a receiver and a multimode optical fibre, characterized in that a multimode optical fibre as described above is used as the multimode optical fibre for a transmission of n×at least 1 Gbit/sec, the distance between the transmitter and the receiver being at least 1 km, wherein n>=2.

In specific embodiments the aforesaid optical communication system is preferably characterized in that a multimode optical fibre as described above is used as the multimode optical fibre for a transmission of n×at least 10 Gbit/sec, the distance between the transmitter and the receiver being at least 150 m, wherein n>=2.

For a special optical communication system, a multimode optical fibre as described above is used as the multimode optical fibre for a transmission capacity of n×at least 1 Gbit/sec, the distance between the transmitter and the receiver being at least 850 m, wherein n>=2.

The parameter “n” is to be understood to mean a multichannel optical communication system, whilst furthermore the present invention also relates to a single-channel optical communication system, wherein the transmission capacity is at least 1 Gbit/sec or 10 Gbit/sec, respectively wherein the transmitter is in particular a laser that is not temperature-stabilized. Depending on the magnitude of the wavelength drift of such lasers without temperature stabilisation, the optical communication systems comprising such lasers may also be configured as multichannel systems.

According to the present invention, the multimode optical fibres can be obtained by using two or more dopants for building up the gradient index core of a multimode optical fibre. By varying the concentration of dopants over the core radius, the intermode dispersion characteristics of the multimode optical fibre can be adapted in such a manner that the bandwidth is less wavelength-dependent. By simultaneously defining a very precise refractive index profile, a high bandwidth is obtained over a wide wavelength range.

Preferably, GeO₂ and F are used as the dopants in SiO₂ for building up the optical core. It is important in this connection that the concentration of F in the optical core of the multimode fibre is lower on the fibre axis (position r=0) than elsewhere in the fibre core (at position 0<r=<a), wherein the edge of the core is defined as r=a. In this way the bandwidth-dependence of the wavelength of the light that is used can be influenced in such a manner that a sufficient production yield of the present fibres can be realised.

Other combinations of dopants in SiO₂ may be used in the same manner for influencing the intermode dispersion characteristics of the optical fibre so that the wavelength-dependence of the bandwidth decreases. The dopants that may be used include, besides the aforesaid GeO₂ and F: B₂O₃, P₂O₅, N, TiO₂, ZrO₂, SnO₂ or Al₂O₃.

Special embodiments of the multimode optical fibre according to the present invention and of the method for manufacturing such a multimode optical fibre are defined in the subclaims.

The present invention will be explained in more detail hereinafter with reference to a number of figures, in which connection it should be noted, however, that the present invention is by no means limited to such a special figure.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows the relation between the wavelength and the bandwidth of a multimode optical fibre according to the prior art.

FIG. 2 shows the refractive index profile and the dopant concentration of the optical fibre that is shown in FIG. 1.

FIG. 3 shows the relation between the wavelength and the bandwidth of another multimode optical fibre according to the present invention.

FIG. 4 shows the refractive index profile and the dopant concentration of the multimode optical fibre that is shown in FIG. 3.

FIG. 5 shows the relation between the wavelength and the bandwidth of yet another multimode optical fibre according to the present invention.

FIG. 6 shows the refractive index profile and the dopant concentration of the multimode optical fibre that is shown in FIG. 5.

DETAILED DESCRIPTION

FIG. 1 shows the wavelength-dependence of the bandwidth of a multimode optical fibre as known from the prior art. The refractive index profile (full line) and the concentration of F (broken line) of said fibre are shown in FIG. 2. The concentration of F may vary from 0 to about 4 weight percent, and the refractive index profile is formed by having the concentration of a refractive index-increasing dopant, such as GeO₂, P₂O₅, or combinations thereof, vary along the core radius in accordance with the desired shape of the refractive index profile. The position of the peak of maximum bandwidth in the figure may be shifted to a higher or a lower wavelength by having the concentration of F (which is constant along the radius) increase or decrease or by changing the shape of the refractive index profile, wherein a lower value of the profile parameter α causes the peak to shift to the right. Such shifts of the value of α or of the concentration of F do not lead to significant changes in the shape of the peak that is shown in FIG. 1. Deviations from the ideal refractive index profile according to the formula generally lead to bandwidths that range below the curve of FIG. 1. The curve of FIG. 1 thus shows the maximum bandwidth that can be achieved with a specific wavelength for a fibre of a specific composition.

FIG. 3 shows an example of the bandwidth-dependence of a multimode optical glass fibre for a multimode optical glass fibre having a refractive index profile (full line) and the concentration of F (broken line) according to the principle of FIG. 4. By having the concentration of F increase in radial direction from the central fibre axis, the dispersion characteristics of the multimode optical fibre are influenced to such an extent that a specific minimum bandwidth is available over a larger wavelength range. The width of the peak at half height is 1.8 times the width in FIG. 1. FIG. 4 shows a linear increase of the concentration of F as a function of the radius in the core of the multi-mode optical glass fibre. Such changes in the wavelength-dependence of the bandwidth also occur in the case of parabolic or exponential increases of the concentration of F as a function of the radius, however.

In the example according to FIG. 4, the concentration of F increases from 0 weight percent on the central fibre axis (at r=0) to a maximum value between approximately 0.5 and 5 weight percent at the edge of the optical core (at r=a). By using such a change in the F-dopant concentration e.g. from 0 to 5 weight percent in a standard multimode fibre having a core diameter of 62.5 μm and an NA of about 0.27, an α-value of about 1.97 will result in an optical fibre which is suitable for transmission of at least 1 Gbit/sec over a distance of a 1000 m in a wavelength range comprising 1300 nm. Such a fibre can be used in an optical communication system comprising a transmitter and a receiver, in which simultaneous signal transmission takes place at two or more wavelengths at a transmission rate of at least 1 Gbit/sec over a wavelength band having a width of at least 100 nm for each wavelength over a distance of minimally 1000 m. Such an optical fibre can also be used in an optical communication system comprising a transmitter that is not temperature-stabilised as well as a receiver at a transmission rate of at least 1 Gbit/sec over a distance of at least 1000 m. A similar change in the F-dopant concentration in a standard multimode fibre having a core diameter of 50 μm and an NA of about 0.2, likewise at an α-value of about 1.97, provides a fibre which is suitable for transmission of at least 1 Gbit/sec over a distance of 2000 m in a wavelength band having a width of 100 nm in a wavelength range comprising 1300 nm. Such a fibre can be used in an optical communication system comprising a transmitter and a receiver, in which simultaneous signal transmission takes place at two or more wavelengths at a transmission rate of at least 1 Gbit/sec for each wavelength over a distance of minimally 2000 m. Such a fibre can also be used in an optical communication system comprising a transmitter that is not temperature-stabilized as well as a receiver at a transmission rate of at least 1 Gbit/sec over a distance of at least 2000 m.

The selection of a higher α-value causes the peak of the bandwidth to shift to a lower wavelength. The use of such a change in the F-dopant concentration e.g. from 0 to 1.5 weight percent in a multimode fibre having an α-value of about 2.05 makes it possible to adapt a standard multimode fibre having a core diameter of 62.5 μm and an NA of about 0.27 for transmission of at least 10 Gbit/sec over a distance of 150 m in a wavelength band having a width of 50 nm in a wavelength range comprising 850 nm. A standard multimode fibre having a core diameter of 50 μm and an NA of about 0.2 can thus be adapted for transmission of at least 10 Gbit/sec over a distance of 300 m in a wavelength band having a width of 50 nm in a wavelength range comprising 850 nm. An increase in the difference between the minimum amount of F-dopant and the maximum amount of F-dopant e.g. from 0 to 2 weight percent will result in an extension of the wavelength band within which the fibres are suitable for said transmission rate and said distance. In this case the wavelength band would increase from 50 nm to 100 nm. Said fibres, which are optimised at 850 nm, can be used in an optical communication system comprising a transmitter and a receiver, in which simultaneous signal transmission takes place at two or more wavelengths at a transmission rate of at least 10 Gbit/sec for each wavelength over a distance of at least 150 m. Said fibres can also be used in an optical communication system comprising a transmitter that is not temperature-stabilised as well as a receiver at a transmission rate of at least 10 Gbit/sec over a distance of at least 150 m. It is also possible to obtain the intended effects when using a concentration of F>0 weight percent on the central fibre axis. Thus a change in the concentration of F from 0 to 1 weight percent appears to produce the same results as a change from 0.5 to 1.5 or from 2 to 3 weight percent. A special embodiment is shown in FIG. 6, in which the concentration of F increases in radial direction from the central fibre axis to a specific maximum value of about 0.5-8 weight percent at a radius r_max which ranges between 0 and a, and which subsequently decreases from r_max to a. By using such a special change in the F-dopant concentration, with a maximum concentration of F-dopant between a radius from 0 to a, standard multimode fibres can be adapted for high transmission rates over a large wavelength band, viz. larger than 250 nm. A standard multimode fibre having a core diameter of 62.5 μm and an NA of about 0.27 becomes suitable for transmission of 1 Gbit/sec over a distance of 850 m over a wavelength band of more than 250 nm. By doping said fibres during manufacture thereof with a thus varying F-dopant concentration, wherein a maximum F-dopant concentration of 5 weight percent is used with a radius r=20 μm, for example, and a concentration of F=0 is maintained in the centre of the core and at the edge of the core, and simultaneously co-doping with a changing concentration of GeO₂, it is possible to realise a refractive index profile having a specific α-value. When an α-value of about 2.3 is selected, the wavelength band comprises a width of 250 nm in a wavelength range of 1400 nm.

Similarly, a standard multimode fibre having a core diameter of 50 μm and an NA of about 0.2 is suitable for transmission of 1 Gbit/sec over a distance of 1300 m over a wavelength band of more than 250 nm by doping said fibres during manufacture thereof with such a varying F-dopant concentration, wherein a maximum F-dopant concentration of e.g. 4.5 weight percent is used with r=15 μm, with a refractive index profile having an α-value of about 2.4.

Such fibres can be used in an optical communication system comprising a transmitter and a receiver, in which simultaneous signal transmission takes place at two or more wavelengths at a transmission rate of at least 1 Gbit/sec for each wavelength over a distance of minimally 850 m. Such fibres can also be used in an optical communication system comprising a transmitter that is not temperature-stabilised as well as a receiver at a transmission rate of at least 1 Gbit/sec over a distance of at least 850 m.

The term standard multimode fibre is to be understood to mean a multimode fibre having a core diameter of 50 μm, an OFL-bandwidth of >400 Mhz·km at 850 nm and >400 Mhz·km at 1300 nm; a multimode fibre having a core diameter of 62.5 μm; an OFL-bandwidth of >160 Mhz·km at 850 nm and >300 Mhz·km at 1300 nm.

FIG. 5 shows an example of the bandwidth-dependence of a multimode optical glass fibre for a multimode optical glass fibre comprising a mole fraction GeO₂ (dashed line), a refractive index profile (full line) and a concentration of F (broken line) according to the principle of FIG. 6. In this way it appears to be possible to obtain a specific minimum bandwidth over an even larger wavelength range; the width at half height of the “peak” in FIG. 5 is 10.8 times the width according to the prior art as shown in FIG. 1. Several production processes exist that are capable of incorporating the aforesaid F-dopants in the core of a multimode fibre. Because of the higher incorporation efficiency for fluor, the PCVD process is very suitable for this purpose. In this process, glass layers are deposited on the inside of a substrate tube via a deposition process, which glass layers will form the core of the multimode fibre. The gaseous process gases are supplied at the inlet side of the tube and react to form a thin layer of glass on the inside of the tube under the influence of a reciprocating low-pressure plasma generated in the tube. A thin layer of glass is deposited with every stroke of the plasma. By varying the concentrations of the raw materials in the gas flow being supplied with every stroke, or continuously in time, a refractive index profile comprising one of the varying F-dopant concentrations as described above is obtained. According to the inventors it is also possible to obtain such varying dopant concentrations when using other optical fibre production processes. An example of this is the MCVD process, wherein the gases supplied to the interior of the tube react to form glass layers on the inside of the substrate tube under the influence of an external heat source, wherein the concentration of the raw materials in the gas flow being supplied can be varied with each glass layer that is deposited. The same applies to OVD or VAD. After the deposition of the glass layers, a preform is formed by contracting a hollow tube or sintering the deposited layers of soot. Such a preform is drawn into an optical glass fibre, using heat.

Such multimode optical fibres can also be obtained by using mode coupling. Dutch patent application Ser. No. 1022315 (not pre-published) in the name of the present applicant describes an example of a method in which stress centres are very locally introduced into the fibre, which stress centres arrange for the coupling of the various modes that effect the transmission of the signal in a multimode fibre, so that there will be no differences in the transmission rate of higher-order modes and lower-order modes, and that more or less independently of the refractive index profile. This, too, makes the bandwidth less wavelength-dependent. Also combinations of mode coupling with the doping technique as described above are used in order to obtain multimode optical fibres according to the present invention.

EXAMPLE 1

multimode optical fibre comprising a core having a gradient index of refraction in accordance with equation 1, a core diameter of 50.2 μm and an NA of 0.201 was formed. The value of the profile shape parameter a was 1.97. The concentration of fluor in the core increased from 0 weight percent on the central fibre axis, at r=0, to 4 weight percent at the edge of the core, at r=a.

The bandwidth of said fibre was measured at 850 nm and at a number of wavelengths around 1300 nm, using the method of FOTP-204. The results are presented in the Table 1 (below). Furthermore, the DMD was measured at 1300 nm, the DMD pulse responses did not exhibit any perturbations in the central part.

TABLE 1
Wavelength l [nm]	850	1250	1270	1300	1330	1350
Bandwidth [MHz · km]	447	2037	1979	2280	2027	1829

In the illustrated wavelength range around 1300 nm, a minimum bandwidth of 1821 Mhz·km over the entire wavelength range is required in order to be able to guarantee a transmission rate of at least 1 Gbit/sec over a minimum distance of 2000 m. The bandwidths in the wavelength range around 1300 nm of the fibre are thus sufficiently high for providing said transmission capacity.

COMPARATIVE EXAMPLE 1

A multimode optical fibre comprising a core having a gradient index of refraction in accordance with equation 1, a core diameter of 49.9 μm and an NA of 0.202 was formed. The value of the profile shape parameter a was 1.97. The concentration of fluor in the core was at a constant value of 0.2 weight percent in the fibre core.

The bandwidth of said fibre was measured at 850 nm and at a number of wavelengths around 1300 nm, using the method of FOTP-204. The results are presented in the Table 2 (below). Furthermore, the DMD was measured at 1300 nm, the DMD pulse responses did not exhibit any perturbations in the central part

TABLE 2
Wavelength l [nm]	850	1250	1270	1300	1330	1350
Bandwidth [MHz · km]	324	993	1128	2095	2257	1401

The bandwidth of the fibre at wavelengths of 1300 nm and 1330 nm is sufficiently high for a transmission rate of at least 1 Gbit/sec over minimally 2000 m. At the other wavelengths that are shown in the table, the bandwidth is too low for said transmission capacity.

COMPARATIVE EXAMPLE 2

A multimode optical fibre comprising a core having a gradient index of refraction in accordance with equation 1, a core diameter of 50.4 μm and an NA of 0.206 was formed. The value of the profile shape parameter α was 1.93. The concentration of fluor in the core decreased from 4 weight percent on the central fibre axis, at r=0, to 0 weight percent at the edge of the core, at r=a.

The bandwidth of said fibre was measured at a wavelength of 850 nm and at a number of wavelengths around 1300 nm, using the method of FOTP-204. The results are presented in the Table 3 (below). Furthermore, the DMD was measured at 1300 nm, the DMD pulse responses did not exhibit any perturbations in the central part.

TABLE 3
Wavelength l [nm]	850	1250	1270	1300	1330	1350
Bandwidth [MHz · km]	269	773	1020	2354	1056	629

The bandwidth of the fibre at a wavelength of 1300 nm is sufficiently high for a transmission rate of at least 1 Gbit/sec over minimally 2000 m. At the other wavelengths that are shown in the table, the bandwidth is too low for said transmission capacity, however.

EXAMPLE 2

A multimode optical fibre comprising a core having a gradient index of refraction in accordance with equation 1, a core diameter of 62.3 μm and an NA of 0.269 was formed. The value of the profile shape parameter a was 1.97. The concentration of fluor in the core increased from 0 weight percent on the central fibre axis, at r=0, to 4 weight percent at the edge of the core, at r=a.

The bandwidth of said fibre was measured at a wavelength of 850 nm and at a number of wavelengths around 1300 nm, using the method of FOTP-204. The results are presented in the Table 4 (below). Furthermore, the DMD was measured at 1300 nm, the DMD pulse responses did not exhibit any perturbations in the central part.

TABLE 4
Wavelength l [nm]	850	1250	1270	1300	1330	1350
Bandwidth [MHz · km]	175	720	820	1010	904	817

In the illustrated wavelength range around 1300 nm, a minimum bandwidth of 707 Mhz·km over the entire wavelength range is required in order to be able to guarantee a transmission rate of 1 Gbit/sec over a minimum length of 1000 m. The bandwidths in the wavelength range around 1300 nm of the fibre are thus sufficiently high for providing said transmission capacity

COMPARATIVE EXAMPLE 3

A multimode optical fibre comprising a core having a gradient index of refraction in accordance with equation 1, a core diameter of 62.4 μm and an NA of 0.262 was formed. The value of the profile shape parameter α was 1.96. The concentration of fluor in the core was at a constant value of 1 weight percent in the fibre core.

The bandwidth of said fibre was measured at 850 nm and at a number of wavelengths around 1300 nm, using the method of FOTP-204. The results are presented in the Table 5 (below). Furthermore, the DMD was measured at 1300 nm, the DMD pulse responses did not exhibit any perturbations in the central part.

TABLE 5
Wavelength l [nm]	850	1250	1270	1300	1330	1350
Bandwidth [MHz · km]	273	522	695	955	909	726

In the illustrated wavelength range around 1300 nm, a minimum bandwidth of 707 Mhz·km over the entire wavelength range is required in order to be able to guarantee a transmission rate of at least 1 Gbit/sec over a minimum length of 1000 m. The fibre that is shown here does not have this bandwidth over the entire wavelength range of 1250-1350 nm.

EXAMPLE 3

A multimode optical fibre comprising a core having a gradient index of refraction in accordance with equation 1, a core diameter of 49.7 μm and an NA of 0.198 was formed. The value of the profile shape parameter α was 2.045. The concentration of fluor in the core increased from 0 weight percent on the central fibre axis, at r=0, to 2 weight percent at the edge of the core, at r=a.

The bandwidth of said fibre was measured at a number of wavelengths around 850 nm and at 1300 nm, using the method of FOTP-204. The results are presented in the Table 6 (below). Furthermore, the DMD was measured at 850 nm, the DMD pulse responses did not exhibit any perturbations in the central part.

TABLE 6
Wavelength l [nm]	800	820	850	875	900	1300
Bandwidth [MHz · km]	2182	2604	4880	2791	2081	634

In the illustrated wavelength range around 850 nm, a minimum bandwidth of 2000 Mhz·km over the entire wavelength range is required in order to be able to guarantee a transmission rate of 10 Gbit/sec over a minimum length of 300 m. The bandwidths in the wavelength range around 800 nm of the fibre are thus sufficiently high for providing said transmission capacity.

EXAMPLE 4

A multimode optical fibre comprising a core having a gradient index of refraction in accordance with equation 1, a core diameter of 50.3 μm and an NA of 0.201 was formed. The value of the profile shape parameter α was 2.05. The concentration of fluor in the core increased from 1 weight percent on the central fibre axis, at r=0, to 2.5 weight percent at the edge of the core, at r=a.

The bandwidth of said fibre was measured at a number of wavelengths around 850 nm and at 1300 nm, using the method of FOTP-204. The results are presented in the Table 7 (below). Furthermore, the DMD was measured at 850 nm, the DMD pulse responses did not exhibit any perturbations in the central part.

TABLE 7
Wavelength l [nm]	800	825	850	875	900	1300
Bandwidth [MHz · km]	1829	2737	4860	2652	1789	583

In the illustrated wavelength range around 850 nm, a minimum bandwidth of 2000 Mhz·km over the entire wavelength range is required in order to be able to guarantee a transmission rate of 10 Gbit/sec over a minimum length of 300 m. The bandwidths in a wavelength band having a width of at least 50 nm around 850 nm of the fibre that is shown here are sufficiently high for providing said transmission capacity.

EXAMPLE 5

A multimode optical fibre comprising a core having a gradient index of refraction in accordance with equation 1, a core diameter of 62.7 μm and an NA of 0.274 was formed. The value of the profile shape parameter α was 2.03. The concentration of fluor in the core increased from 0 weight percent on the central fibre axis, at r=0, to 3 weight percent at the edge of the core, at r=a.

The bandwidth of said fibre was measured at a number of wavelengths around 850 nm and at 1300 nm, using the method of FOTP-204. The results are presented in the Table 8 (below). Furthermore, the DMD was measured at 850 nm, the DMD pulse responses did not exhibit any perturbations in the central part.

TABLE 8
Wavelength l [nm]	800	820	850	875	900	1300
Bandwidth [MHz · km]	1135	1542	2056	1814	826	357

In the illustrated wavelength range around 850 nm, a minimum bandwidth of 808 Mhz·km over the entire wavelength range is required in order to be able to guarantee a transmission rate of 10 Gbit/sec over a minimum length of 150 m. The bandwidths in a wavelength band having a width of at least 100 nm around 850 nm of the fibre that is shown here are sufficiently high for providing said transmission capacity.

EXAMPLE 6

A multimode optical fibre comprising a core having a gradient index of refraction in accordance with equation 1, a core diameter of 49.7 μm and an NA of 0.198 was formed. The value of the profile shape parameter α was 2.427. The concentration of fluor in the core increased from 0 weight percent on the central fibre axis, at r=0, to a maximum value of 6.1 weight percent at r=15.5, after which the concentration of fluor decreased to a value of 0 weight percent at the edge of the core, at r=a.

The bandwidth of said fibre was measured at a number of wavelengths between 1300 nm and 1550 nm and at 850 nm, using the method of FOTP-204. The results are presented in the Table 9 (below). Furthermore, the DMD was measured at 1300 nm, the DMD pulse responses did not exhibit any perturbations in the central part.

TABLE 9
Wavelength l [nm]	850	1300	1360	1400	1450	1500	1550
Bandwidth	431	1477	1386	1597	1537	1344	1529
[MHz · km]

In the wavelength range around 1400 nm and especially in the illustrated wavelength range from 1300 nm to 1550 nm, a minimum bandwidth of 1196 Mhz·km over the entire wavelength range is required in order to be able to guarantee a transmission rate of at least 1 Gbit/sec over a minimum length of 1300 m. The bandwidths in a wavelength range around 1400 nm of the fibre are thus sufficiently high for providing said transmission capacity.

EXAMPLE 7

A multimode optical fibre as mentioned in Example 6 was formed, except that the value of the profile shape parameter α was 2.28 and the maximum concentration of fluor was 5.4 weight percent.

The bandwidth of said fibre was measured at a number of wavelengths between 1200 nm and 1450 nm, using the method of FOTP-204. The results are presented in the Table 10 (below). Furthermore, the DMD was measured at 1300 nm, the DMD pulse responses did not exhibit any perturbations in the central part.

TABLE 10
Wavelength l [nm]	850	1200	1230	1300	1360	1400	1450
Bandwidth	546	1217	1356	1267	1369	1382	1275
[MHz · km]

In the wavelength range around 1400 nm and especially in the illustrated wavelength range from 1200 nm to 1450 nm, a minimum bandwidth of 1100 Mhz·km over the entire wavelength range is required in order to be able to guarantee a transmission rate of at least 1 Gbit/sec over a minimum length of 1300 m. The bandwidths in the wavelength range around 1400 nm of the fibre are thus sufficiently high for providing said transmission capacity.

Claims

1. A method for manufacturing a multimode optical fibre having a refractive index profile, comprising: supplying a reactive gas mixture of doped or undoped glass-forming gases to the interior of a substrate tube using a chemical vapour deposition technique;forming one or more glass layers on the interior of the substrate tube;contracting the substrate tube to yield an optical preform having a precisely defined refractive index profile;heating one end of the optical preform; anddrawing from the heated end of the preform a multimode optical fibre comprising a gradient index light-guiding core surrounded by one or more cladding layers, wherein the gradient index light-guiding core comprises at least one refractive index-changing dopant with a concentration increasing in a radial direction from a fibre axis (r=0).

2. A method according to claim 1, wherein the concentration of at least one refractive index-changing dopant in the gradient index light-guiding core increases in the radial direction from about 0 weight percent at the fibre axis (r=0) to about 6.5 weight percent.

3. A method according to claim 1, wherein the concentration of at least one refractive index-changing dopant in the gradient index light-guiding core increases in the radial direction from the fibre axis (r=0) to a maximum value at a radial position (rmax) between the fibre axis (r=0) and the outer edge of the optical core (r=a).

4. A method according to claim 1, wherein at least one refractive index-changing dopant in the gradient index light-guiding core comprises GeO2, F, B2O3, P2O5, N, TiO2, ZrO2, SnO2 and/or Al2O3.

5. A method according to claim 1, wherein at least one refractive index-changing dopant in the gradient index light-guiding core includes GeO2 and F.

6. A method according to claim 1, wherein: the gradient index light-guiding core includes fluorine; andthe multimode optical fiber has a transmission capacity of at least 1 Gbit/sec over a fibre length of at least 1300 m, and a wavelength bandwidth of at least 250 nm in a wavelength range including 1400 nm.

7. A method according to claim 6, wherein the multimode optical fiber has an optical core diameter of 50 μm.

8. A method according to claim 6, wherein the multimode optical fiber has a numerical aperture of between about 0.18 and 0.22.

9. A method according to claim 6, wherein the multimode optical fiber has a minimum OFL bandwidth of at least 400 Mhz·km at 850 nm.

10. A method according to claim 6, wherein the multimode optical fiber has minimum OFL bandwidth of at least 400 Mhz·km at 1300 nm.

11. A method for manufacturing a multimode optical fibre having a refractive index profile, comprising: supplying a reactive gas mixture of doped or undoped glass-forming gases to the interior of a substrate tube using a chemical vapour deposition technique;forming one or more glass layers on the interior of the substrate tube;contracting the substrate tube to yield an optical preform having a precisely defined refractive index profile;heating one end of the optical preform; anddrawing from the heated end of the preform a multimode optical fibre comprising a gradient index light-guiding core surrounded by one or more cladding layers, wherein (i) the gradient index light-guiding core includes fluorine having a concentration that increases in a radial direction from a fibre axis (r=0), and (ii) the multimode optical fiber has a transmission capacity of at least 1 Gbit/sec over a fibre length of at least 850 m and a wavelength bandwidth of at least 250 nm in a wavelength range including 1400 nm.

12. A method according to claim 11, wherein the fluorine concentration on the fibre axis (r=0) is lower than the fluorine concentration in a region of the gradient index light-guiding core.

13. A method according to claim 11, wherein the fluorine concentration within the gradient index light-guiding core increases from about 0 weight percent at the fibre axis (r=0) to between about 0.5 and 5 weight percent at the edge of the optical core (r=a).

14. A method according to claim 11, wherein the fluorine concentration within the gradient index light-guiding core increases linearly in a radial direction from the fibre axis (r=0) as a function of optical core radius.

15. A method according to claim 11, wherein the fluorine concentration within the gradient index light-guiding core increases non-linearly in a radial direction from the fibre axis (r=0) as a function of optical core radius.

16. A method according to claim 11, wherein the fluorine concentration within the gradient index light-guiding core increases in a radial direction from the fibre axis (r=0) as an exponential function of optical core radius.

17. A method according to claim 11, wherein the fluorine concentration within the gradient index light-guiding core increases in a radial direction from the fibre axis (r=0) as a parabolic function of optical core radius.

18. A method according to claim 11, wherein the fluorine concentration within the gradient index light-guiding core increases in a radial direction from the fibre axis (r=0) to its maximum value at a radial position (rmax) between the fibre axis (r=0) and the edge of the optical core (r=a).

19. A method according to claim 18, wherein the fluorine concentration within the gradient index light-guiding core decreases in a radial direction from rmax to the edge of the optical core (r=a).

20. A method according to claim 11, wherein the fluorine concentration within the gradient index light-guiding core increases in a radial direction from the fibre axis (r=0) to a maximum value of between about 0.5 and 8 weight percent at a radial position (rmax) between the fibre axis (r=0) and the edge of the (optical) core (r=a).

21. A method according to claim 20, wherein the fluorine concentration within the gradient index light-guiding core increases from about 0 weight percent at the fibre axis (r=0) to a maximum value of between about 0.5 and 6 weight percent.

22. A method according to claim 11, wherein the fluorine concentration within the gradient index light-guiding core is negligible both at the fibre axis (r=0) and at the edge of the (optical) core (r=a).

23. A method according to claim 11, wherein the gradient index light-guiding core further includes at least one additional refractive-index-changing dopant.

24. A method according to claim 11, wherein the multimode optical fiber has an optical core diameter of 62.5 μm.

25. A method according to claim 11, wherein the multimode optical fiber has a numerical aperture of between about 0.25 and 0.30.

26. A method according to claim 11, wherein the multimode optical fiber has a minimum OFL bandwidth of at least 160 Mhz·km at 850 nm.

27. A method according to claim 11, wherein the multimode optical fiber has a minimum OFL bandwidth of at least 300 Mhz·km at 1300 nm.

28. A method for manufacturing an optical fiber preform having an improved refractive index profile, comprising: providing a glass substrate tube;supplying reactive gas mixtures of glass-forming gases to the interior of the substrate tube to form a plurality of deposited cladding layers on the substrate tube's interior surface;thereafter supplying a reactive gas mixture of fluorine-containing, glass-forming gases to the interior of the substrate tube to form a plurality of deposited core layers, wherein, during the formation of the innermost deposited core layer, the concentration of fluorine in the reactive gas mixture decreases from its concentration during the formation of the immediately preceding core layer; andcontracting the substrate tube to yield the optical preform having a precisely defined refractive index profile.

29. A method according to claim 28, wherein during the step of supplying a reactive gas mixture of fluorine-containing, glass-forming gases to the interior of the substrate tube to form a plurality of deposited core layers, the concentration of fluorine in the reactive gas mixture is negligible during the formation of the innermost deposited core layer.

30. A method according to claim 28, wherein during the step of supplying a reactive gas mixture of fluorine-containing, glass-forming gases to the interior of the substrate tube to form a plurality of deposited core layers, the concentration of fluorine in the reactive gas mixture changes as a parabolic function of the deposition thickness of the deposited core layers.

31. A method for manufacturing an optical fiber preform having an improved refractive index profile, comprising: providing a glass substrate tube;supplying reactive gas mixtures of glass-forming gases to the interior of the substrate tube to form a plurality of deposited cladding layers on the substrate tube's interior surface;thereafter supplying a reactive gas mixture of fluorine-containing, glass-forming gases to the interior of the substrate tube to form an outermost deposited core layer on the innermost deposited cladding layer, wherein the reactive gas mixture contains sufficient fluorine to achieve an outermost deposited core layer having between about 0.5 and 5 weight percent fluorine;continuing to supply reactive gas mixtures of fluorine-containing, glass-forming gases to the interior of the substrate tube to form a plurality of deposited core layers, wherein the concentration of fluorine present in the reactive gas mixtures of fluorine-containing glass-forming gases changes as a function of the core deposition thickness; andthereafter contracting the glass substrate tube to yield an optical preform having a refractive index profile in which the fluorine concentration generally increases in a radial direction from an innermost deposited core layer to the outermost deposited core layer.

32. A method according to claim 31, wherein the concentration of fluorine present in the reactive gas mixtures of fluorine-containing, glass-forming gases generally decreases in relation to the deposition thickness of the deposited core layers.

33. A method according to claim 32, wherein during the formation of the innermost deposited core layer the concentration of fluorine present in the reactive gas mixtures is about 0 weight percent.

34. A method according to claim 31, wherein, during the step of continuing to supply reactive gas mixtures to the interior of the substrate tube, the concentration of fluorine present in the reactive gas mixtures of fluorine-containing, glass-forming gases generally decreases linearly in relation to the deposition thickness of the deposited core layers.

35. A method according to claim 31, wherein, during the step of continuing to supply reactive gas mixtures to the interior of the substrate tube, the concentration of fluorine present in the reactive gas mixtures of fluorine-containing, glass-forming gases decreases from between about 0.5 and 5 weight percent at the outermost deposited core layer to about 0 weight percent at the innermost deposited core layer.

36. A method according to claim 31, wherein, during the step of continuing to supply reactive gas mixtures to the interior of the substrate tube, the concentration of fluorine present in the reactive gas mixtures of fluorine-containing, glass-forming gases generally decreases non-linearly in relation to the deposition thickness of the deposited core layers.

37. A method according to claim 31, wherein, during the step of continuing to supply reactive gas mixtures to the interior of the substrate tube, the concentration of fluorine present in the reactive gas mixtures of fluorine-containing, glass-forming gases generally decreases exponentially in relation to the deposition thickness of the deposited core layers.

38. A method according to claim 31, wherein, during the step of continuing to supply reactive gas mixtures to the interior of the substrate tube, the concentration of fluorine present in the reactive gas mixtures of fluorine-containing, glass-forming gases generally decreases parabolically in relation to the deposition thickness of the deposited core layers.

39. A method according to claim 31, wherein, during the step of continuing to supply reactive gas mixtures to the interior of the substrate tube, the concentration of fluorine present in the reactive gas mixtures of fluorine-containing, glass-forming gases decreases from a maximum of between about 0.5 and 8 weight percent at an inner deposited core layer (rmax) toward the innermost deposited core layer (r=0).

40. A method according to claim 31, wherein, during the step of continuing to supply reactive gas mixtures to the interior of the substrate tube, the concentration of fluorine present in the reactive gas mixtures of fluorine-containing, glass-forming gases decreases from a maximum of between about 0.5 and 6 weight percent toward the innermost deposited core layer (r=0).

41. A method according to claim 31, wherein the fluorine concentration within the gradient index light-guiding core is negligible both at the innermost deposited core layer (r=0) and at the outermost deposited core layer (r=a).

42. A method according to claim 31, wherein the step of continuing to supply reactive gas mixtures to the interior of the substrate tube comprises supplying a reactive gas mixture of glass-forming gases that include fluorine and at least one additional refractive-index-changing dopant.